
where \(\omega _{i}=m_{i}/(m_{i}+m_{j})\) . In above Lagrangians, the effective correlation function \(\Phi (y^2)\)  show the distribution of the componenets
in the hadronic molecule \(P_{cs}(4459)\)  state. Moreover, the role of the correlation function \(\Phi (y^2)\)  also is to avoid the Feynman diagrams
ultraviolet divergence and his Fourier transform should vanish quickly in the ultraviolet region in the Euclidean space. We adopt the form as
used in Refs. [1]}, [2]}
\(\Phi (-p^2)\doteq {}\exp (-p_E^2/\Lambda ^2),\) 
